The Linearized Einstein Equations with Sources on Compact Riemannian Manifolds With Boundary
Roee Leder
TL;DR
The paper addresses the solvability and uniqueness of the linearized Einstein equations with sources on compact Riemannian manifolds with boundary under a Ricci-boundary constraint. It introduces lifted divergence $\textdelta_g$ and a lifted Einstein operator $\mathpzc{D}_{\Gamma}\mathpzc{Ein}_g$, assembling them within a generalized Hodge theory framework on manifolds with boundary via the Boutet de Monvel calculus. The main result characterizes solvability by the conditions $\textdelta_g T = 0$ and $T|_{\partial M}=0$, with the solution unique modulo finite-dimensional obstructions captured by a lifted cohomology; in the typical boundary setting these obstructions vanish, yielding convergence to solvability. The approach blends Green's formulae, Hodge decompositions, and a unique continuation lemma (Aronszajn–Cordes) to remove interior/topological restrictions and to enable a linear-to-nonlinear perturbation strategy for Einstein equations with rough interior geometry. The methods extend Lorentzian results to a Riemannian interior, offering a robust linear framework for handling Einstein equations with boundary data and arbitrary interior geometry.
Abstract
We consider compact Riemannian manifolds with arbitrary interior geometry, assuming only that the Ricci tensor vanishes on the boundary. In this setting, we prove that, under the linear Bianchi gauge and extended Cauchy data, the linearized Einstein equations with sources are globally solvable if and only if the source lies in the kernel of a lifted divergence operator and vanishes on the boundary; the solution is unique. This is the first result of its kind without rigid structural restrictions on topology, geometry, or source. The proof combines generalized Hodge theory with unique continuation results.
